Skip to content
DraconiticResearch
Search Sources API
197,788 studies31 sourcesUpdated 24 min ago
PreprintCC BY 4.0arXiv

Schwinger-Keldysh effective field theory of type-B Goldstone: near-diagonal geometry and Berry term

Abstract

In this work, we formulate a finite temperature Schwinger-Keldysh effective field theory for type-B Goldstone modes based on geometric objects globally defined on the coset manifold. In particular, after taking the classical limit, we organize the required two time contour structure by a near-diagonal geometry in which the r-type field is interpreted as the physical Goldstone configuration and the a-type field is identified as corresponding tangent displacement. Within this geometric viewpoint, the Berry term essential for type-B Goldstones is obtained directly through the transgression of the Berry curvature. Moreover, we show that this exact Berry transgression is compatible with dynamical KMS condition. In order to construct the conservative, dissipative and noise sectors, we classify possible tensors globally defined on the coset manifold. Based on this framework, we discuss in detail two concrete model examples. The dispersion relations of the Goldstone modes and the associated two-point correlation functions are calculated in the presence of dissipation.

Related

  1. The price of locality: Maxwell-Cattaneo charge transport in Schwinger-Keldysh effective field theory
    Andrea Amoretti, Matteo Anselmi, Daniel K. Brattan
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsStatistical & nonlinear physicsarXiv
  2. Schwinger-Keldysh effective actions for non-hydrodynamic poles and branch cuts
    Andrea Amoretti, Matteo Anselmi, Daniel K. Brattan
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsStatistical & nonlinear physicsarXiv
  3. A stationary composition law for Schwinger-Keldysh effective actions
    Denis Comelli
    Journal of High Energy PhysicsPeer-reviewedCC BY 4.0Full textHigh-energy & particle physicsSpringerCrossref
  4. Schwinger--Keldysh worldline effective field theory for quantum black holes: dissipation, noise and decoherence
    Hajime Kobayashi
    arXivPreprintCC BY 4.0Full textGravitation & general relativityHigh-energy & particle physicsarXiv
  5. Staying positive: bounds for non-Gaussian noise in Schwinger-Keldysh effective field theory
    Andrea Amoretti, Daniel K. Brattan
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsStatistical & nonlinear physicsarXiv
BibTeX
@misc{zheng2026schwingerkeldysh,
  title = {{Schwinger-Keldysh effective field theory of type-B Goldstone: near-diagonal geometry and Berry term}},
  author = {Pei Zheng and Mei Huang},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2608.09776},
  eprint = {2608.09776},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2608.09776},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Schwinger-Keldysh effective field theory of type-B Goldstone: near-diagonal geometry and Berry term
AU  - Pei Zheng
AU  - Mei Huang
PY  - 2026
DA  - 2026/09/30
PB  - arXiv
DO  - 10.48550/arxiv.2608.09776
UR  - https://arxiv.org/abs/2608.09776
AB  - In this work, we formulate a finite temperature Schwinger-Keldysh effective field theory for type-B Goldstone modes based on geometric objects globally defined on the coset manifold. In particular, after taking the classical limit, we organize the required two time contour structure by a near-diagonal geometry in which the r-type field is interpreted as the physical Goldstone configuration and the a-type field is identified as corresponding tangent displacement. Within this geometric viewpoint, the Berry term essential for type-B Goldstones is obtained directly through the transgression of the Berry curvature. Moreover, we show that this exact Berry transgression is compatible with dynamical KMS condition. In order to construct the conservative, dissipative and noise sectors, we classify possible tensors globally defined on the coset manifold. Based on this framework, we discuss in detail two concrete model examples. The dispersion relations of the Goldstone modes and the associated two-point correlation functions are calculated in the presence of dissipation.
ER  -